Ir supercontinuum source using low-loss heavy metal oxide glasses

ABSTRACT

An IR supercontinuum source for generating supercontinuum in the MIR or possibly LWIR spectral bands comprises a supercontinuum fiber formed from a heavy metal oxide host glass having low optical loss and high non-linearity over the spectral band that is stable, strong and chemically durable. The supercontinuum fiber is suitably a depressed inner clad fiber configured to support only single transverse spatial mode propagation of the pump signal and supercontinuum. The source suitably includes a tapered depressed inner clad fiber to couple the pump signal into the supercontinuum fiber. The source may be configured as an “all-fiber” source.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims benefit of priority under 35 U.S.C. 120 as acontinuation-in-part application of co-pending U.S. patent applicationSer. No. 13/745,028 entitled “Low-Loss UV To MID IR Optical TelluriumOxide Glass and Fiber for Linear, Non-Linear and Active Devices” andfiled on Jan. 18, 2013, the entire contents of which are incorporated byreference.

GOVERNMENT RIGHTS

This invention was made with United States Government support underContract Number N68335-11-C-0035 with the Naval Air Warfare Center AD(LKE). The United States Government has certain rights in thisinvention.

BACKGROUND OF THE INVENTION

1. Field of the Invention

This invention relates to supercontinuum generation, and moreparticularly to an IR supercontinuum source using low-loss heavy metaloxide glasses.

2. Description of the Related Art

Broadband light sources have a wide range of applications in opticalsystems and particularly fiber optic systems. These sources may be usedto generate wavelength division multiplexed (WDM) signals or for opticalspectroscopy of materials, fiber-optic sensing, optical coherencetomography (OCT), fiber optic gyroscopes, frequency metrology, opticalcomponent testing, dispersion characterization of specialty fibers, andoptical interrogation of fiber bragg gratings. Conventional broadbandlight sources include superluminescent semiconductor diodes, rare-earthdoped ASE sources, optical parametric amplifiers, quantum cascade laser,free electron lasers and supercontinuum sources. These sources areevaluated based on many factors including output spatial mode, opticalbandwidth, spectral power density, flatness of the output power over thebandwidth, the temporal pulse width, the energy per pulse, therepetition rate, the time-averaged output power over the bandwidth, theefficiency of the source, and the cost, size, weight, and reliability.

In a supercontinuum source, an optical pump signal interactsnon-linearly with a medium such as an optical fiber to produce newfrequencies leading to significant spectral broadening of the originalpump signal. The pump signal is typically injected into the medium inthe form of optical pulses having pulse widths on the order ofpico-seconds or femto-seconds and high peak power.

Supercontinuum generation is possible in step-index optical fiber ordispersion shifted fiber. However, to achieve maximum supercontinuumbandwidth and the lowest pump power threshold for supercontinuumgeneration, the pump wavelength must be near the zero dispersionwavelength (ZDW) of the fiber. The waveguide structure of the fiber maybe configured to shift the ZDW of the fiber away from the zero materialdispersion wavelength (ZMDW) of the bulk glass to the pump wavelength.Photonic crystal fiber (PCF) is widely used over conventional solidcore/clad fiber in that the dispersion properties of PCF can be easilytailored by manipulating the microstructure.

Supercontinuum generation has been demonstrated in silica photoniccrystal fiber in the visible (0.39-0.75 microns) and near infrared (NIR)(0.75-2 microns). In silica photonic crystal fiber the multiphonon edgeof silica glass limits the transmission window in the IR. This, in turn,limits the extent of spectral broadening in the IR. Supercontinuumsources on the market today such as from Fianium Ltd, NKT Photonics,Leukos, provide a supercontinuum in the visible and NIR that spans fromabout 400 nm to about 2.2 microns.

Many applications exist for broadband sources beyond about 2 micronsinto the Mid IR (MIR) from 2-5 microns and possibly Long Wave IR (LWIR)above 5 microns. Mid-infrared sources are key enabling technology forvarious applications such as remote chemical sensing, defensecommunications and countermeasures, and bio-photonic diagnostics andtherapeutics. Researchers have experimented with other glasses such asfluorides, oxyfluorides, chalcogenides and heavy metal oxides such astellurium oxide to generate supercontinuum into the MIR range. Thenon-linearity of these glasses is typically much greater than that ofsilica based glasses. These researchers have demonstrated supercontinuumgeneration above 2 microns with these glasses. However, the lossesexhibited by these glasses in the upper MIR wavelengths from about 3 toabout 5 microns persist at levels that are too high for uniform andefficient supercontinuum generation. To date, no one has demonstrated asupercontinuum source that generates supercontinuum over the MIR bandfrom about 2 to about 5 microns with sufficient flatness andtime-averaged power over the band to be commercially viable.

SUMMARY OF THE INVENTION

The following is a summary of the invention in order to provide a basicunderstanding of some aspects of the invention. This summary is notintended to identify key or critical elements of the invention or todelineate the scope of the invention. Its sole purpose is to presentsome concepts of the invention in a simplified form as a prelude to themore detailed description and the defining claims that are presentedlater.

The present invention provides an IR supercontinuum source thatgenerates supercontinuum over a spectral band whose upper edge is atleast 3.5 microns using low-loss heavy metal oxide glasses to form thesupercontinuum fiber.

In an embodiment, this is accomplished by removing or reducing glassconstituents that have unwanted absorption features below the upper edgeof the IR spectral band from the core glass in the supercontinuum fiberwhile simultaneously providing glass stability, strength, and chemicaldurability. The glass formulation only includes glass constituents thatprovide the network former, intermediate or modifier, and any halides(for OH— reduction) and any other glass constituent (present in amountsof at least 0.2 mole percent) whose absorption wavelength correspondingto an energy of the third phonon peak is approximately at or longer thanthe edge of the IR spectral band. In an embodiment, the intermediate ormodifier, any halide and any other constituent are selected such thattheir absorption wavelength corresponding to the third phonon peak islonger than that of the network former so that the glass formulationexhibits optical performance as close as possible to the theoreticallimit of the network former. The glass formulation preferably includesat most only a small residual amount of halide. The pre-melt glassformulation suitably includes only a sufficient amount of halide (e.g.Fluoride) to react with and carry away the hydroxyl during the melt. Anon-zero residual amount of halide in the glass indicates thatsubstantially all of the hydroxyl is removed. A small residual amount ofhalide does not degrade the chemical durability of the glass nor does itlead to breakage of heavy metal oxygen bonds that would increaseabsorption in the IR spectral band and weaken the glass.

In an embodiment, a core heavy metal oxide glass comprises a networkformer of 45 to 90) mole percent of an oxide formed from Tellurium (Te),Lead (Pb), Tungsten (W), Tantalum (Ta), Bismuth (Bi), Gallium (Ga).Antimony (Sb), Arsenic (As), Germanium (Ge) or Niobium (Nb) orcombinations thereof, 0.2 to 45 mole percent of an oxide formed from anintermediate of Lanthanum (La), Tungsten (W), Thallium (Tl), Yttrium(Y), Tantalum (Ta), Bismuth (Bi), Gallium (Ga), Antimony (Sb), Arsenic(As). Niobium (Nb), Germanium (Ge), Titanium (Ti) or Zirconium (Zr) orcombinations thereof or a modifier Magnesium (Mg), Calcium (Ca),Strontium (Sr), Barium (Ba), Zinc (Zn), Lead (Pb) or Cadmium (Cd) orcombinations thereof, and a halide of 0 to 15 mole percent. To ensurelow loss in the spectral band, the network former, intermediate ormodifier, and any said halide any other glass constituent (present inmore than trace amounts) each have an absorption wavelengthcorresponding to an energy of the third phonon peak that isapproximately at or longer than the edge the IR spectral band.Additionally, the heavy metal oxide glass is substantially free ofHydroxide (OH—).

In an embodiment in which the upper edge of the source's spectral bandis approximately 5 microns, the core heavy metal oxide glass comprises anetwork former of 45 to 90 mole percent of an oxide formed fromTellurium (Te), said Tellurium oxide having an absorption feature withan absorption wavelength corresponding to an energy of the third phononpeak that is longer than 5 microns, a glass intermediate of 0.2 to 45mole percent of an oxide formed from Lanthanum (La), a glass modifier of0.2 to 45 mole percent of an oxide formed from Mg, Ca, Sr, Ba, Zn, Pband Cd or combinations thereof, and a halide of 0 to 5 mole percent. Theintermediate and modifier, any halide, and any other glass constituenteach have an absorption wavelength corresponding to an energy of thethird phonon peak that is longer than that of the Tellurium oxide. In anembodiment, the Lanthanum oxide concentration is at least 5 molepercent, the halide comprises a non-zero amount of Fluoride less than0.5 mole percent, and the modifier MO comprises ZnO wherein said oxideglass exhibits an optical loss of less than 0.3 dB/m over a spectralsub-range from 2 microns to 4 microns, wherein the source produces anintegrated average output power of at least 10 mW over 4 to 5 microns.

In an embodiment in which the upper edge of the source's spectral bandis at least approximately 7 microns, the network former is a combinationof lead (Pb) and bismuth (Bi) oxide.

In an embodiment in which the upper edge of the source's spectral bandis at least approximately 6.5 microns, the network former is one ofPb/Bi, Pb/Ga or Pb/Ga/Bi.

In an embodiment in which the upper edge of the source's spectral bandis at least approximately 5.5 microns, the network former is one ofPb/Bi, Pb/Ga, Pb/Ga/Bi or Ta/Ga.

In an embodiment in which the upper edge of the source's spectral bandis at least approximately 5 microns, the network former is one of Pb/Bi,Pb/Ga, Pb/Ga/Bi, Ta/Ga, K/La/Ga or Te.

In an embodiment, the supercontinuum fiber comprises a depressed innerclad fiber configured to shift the ZDW of the fiber and supportpropagation of the optical pulsed pump signal in only a singletransverse spatial mode to interact nonlinearly with the core glass andgenerate supercontinuum light over the IR spectral band that propagatesin only a single transverse spatial mode.

In an embodiment, the pump produces the optical pulsed pump signal witha first mode field diameter (MFD) and the supercontinuum fiber receivesthe optical pulsed pump signal with a smaller second MFD. A couplercomprises a depressed inner clad fiber that is fusion spliced betweenthe pump and supercontinuum fiber to taper the MFD from approximatelythe first MFD down to approximately the smaller second MFD. The diameterof the fiber core is physically tapered so that twice the radius at theinput to the coupler approximately equals the first MFD and twice theradius at the output from the coupler approximately equals the secondMFD. The fiber is configured with indices of refraction that define anumerical aperture to support propagation of the optical signal in onlya single transverse spatial mode within the spectral band. The length ofthe physical taper is configured so that the MFD tapers smoothly (e.g.adiabatically) from approximately the first MFD to approximately thesecond MFD to reduce loss of the optical signal into the cladding as theoptical signal propagates through the coupler. The fiber is furtherconfigured with index of refraction n1 and a first cladding diameterthat tapers from a diameter b to b′ so that the taper of the MFDapproximates the physical taper of the core to reduce loss of theoptical signal into the cladding as the optical signal propagatesthrough the coupler.

In an embodiment, the supercontinuum source is configured as anall-fiber source. An all-fiber approach to generate a high power, singlemode beam with extremely wide (e.g. 2 μm-5 μm) and simultaneouswavelength coverage has significant advantages in terms of reliability(no moving parts or alignment), room temperature operation, size,weight, and power efficiency.

These and other features and advantages of the invention will beapparent to those skilled in the art from the following detaileddescription of preferred embodiments, taken together with theaccompanying drawings, in which:

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a block diagram of an IR supercontinuum source;

FIG. 2 is a plot of transmission versus wavelength for different heavymetal oxide glasses;

FIGS. 3 a and 3 b are plots of supercontinuum output power for high andlow loss heavy metal oxide glasses, respectively;

FIGS. 4 a and 4 b are respectively a table of phonon energies andabsorption wavelengths for glass constituents and a diagram of themultiphonon edge;

FIG. 5 is a process diagram for an embodiment of forming a bulk heavymetal oxide glass and then drawing a fiber;

FIG. 6 is a diagram of a tellurium oxide glass composition in accordancewith the present invention;

FIG. 7 is a plot of absorption coefficient versus wavelength fordifferent tellurium oxide glasses;

FIGS. 8 a and 8 b are plots of transmission and propagation loss,respectively versus wavelength for a fiber having a core tellurium oxideglass composition in accordance with the present invention;

FIGS. 9 a and 9 b are diagrams of an embodiment of supercontinuum fiberhaving a depressed inner clad configuration;

FIGS. 10 a and 10 b are plots illustrating the dispersion flattening andshifting properties of the depressed inner clad fiber;

FIGS. 11 a and 11 b are plots illustrating the strong confinement of thelight fields for the pump signal and the generated supercontinuum in asingle transverse spatial mode;

FIG. 12 is a diagram of a tapered fiber coupler for coupling the pumpsignal to the supercontinuum fiber;

FIG. 13 is a flow diagram of an embodiment of a method for designing thetapered fiber coupler, and

FIGS. 14 a and 14 b are plots illustrating the strong confinement of thelight fields for the pump signal in a single transverse spatial mode indifferent MFDs at opposite ends of the coupler.

DETAILED DESCRIPTION OF THE INVENTION

The present invention describes an IR supercontinuum source forgenerating supercontinuum in the MIR or possibly LWIR spectral bands.The source comprises a supercontinuum fiber formed from a heavy metaloxide host glass having low optical loss and high non-linearity over thespectral band that is stable, strong and chemically durable. Thesupercontinuum fiber is suitably a depressed inner clad fiber (aka a“W-fiber” or “Multi-clad fiber”) configured to support only singletransverse spatial mode propagation of the pump signal andsupercontinuum. The source suitably includes a tapered depressed innerclad fiber to couple the pump signal into the supercontinuum fiber. Thesource may be configured as an “all-fiber” source.

Referring now to FIG. 1, an embodiment of a supercontinuum source 10comprises a supercontinuum fiber 12 having an optical non-linearitysufficient for supercontinuum generation, a pump 14 configured toproduce an optical pulsed pump signal, a coupler 16 configured to couplethe pulsed pump signal to the supercontinuum fiber 12, and a collimator18. The supercontinuum fiber is configured to propagate the pulsed pumpsignal to interact nonlinearly with the supercontinuum fiber core togenerate supercontinuum light 20 that spans a defined spectral bandhaving an upper edge of at least 3.5 microns. The band may cover the MIRof 2-5 um, a portion of the MIR whose upper edge is at least 3.5microns, a broader band including the MIR or a portion of the LWIR above5 microns.

In general, supercontinuum fiber 12 must exhibit a wide transparencycovering the defined spectral band (e.g. MIR), low impurity absorptionin the band and low OH— incorporation, high non-linearity coefficientand high conversion efficiency. The fiber suitably supports a wide rangeof refractive indices based on the glass composition to enable a widerange of numerical apertures (NAs). The fiber suitably supports a widerange of fiber core/clad diameters. For example, core diameters of1.5-25 microns and cladding diameters of 77 to 250 microns. Theseproperties are a function of the host glass and the waveguide structureof the fiber. The network former, intermediate and/or modifier, and anyhalide for Hydroxide (OH—) reduction or any other glass constituent(present in more than trace amounts) are selected so that theirabsorbing wavelength of the energy of the third phonon peak is longerthan the longest wavelength in the spectral band. Consequently themulti-phonon edge associated with the host glass is positioned above thespectral band. In other words, the “in-band” absorption of themultiphonon edge is less than a specified threshold absorption.Furthermore, the host glass is substantially free (e.g. <0.1 mole %) ofHydroxide. It is not sufficient to simply reduce the Hydroxide levels,it is important that the glass is substantially free of Hydroxide togenerate supercontinuum in the MIR band. In certain embodiments thehydroxyl content will be less than 0.01 mole % or even 0.001 mole %.Details of the glass formulation and an embodiment of a Tellurium oxideglass will be described in reference to FIGS. 2, 3 a-3 b, 4 a-4 b, 5, 6,7 and 8 a-8 b.

Supercontinuum fiber 12 may be a step-index optical fiber or adispersion shifted fiber. The pump wavelength must be near the zerodispersion wavelength (ZDW) of the fiber to maximize efficiency. Oneoption is to configure the pump to produce the optical pump signal atthe ZDW of a normal step-index optical fiber. Another option is to shiftthe ZDW of the fiber to a desirable pump wavelength. Photonic crystalfiber (PCF) is widely used over conventional core/clad fiber in that thedispersion properties of PCF can be easily tailored by manipulating themicrostructure. Alternately, a depressed inner clad fiber can be used totailor the dispersion properties to shift the ZDW. The supercontinuumfiber may support propagation of the pump signal and supercontinuum ineither single or multiple transverse spatial modes. As will be describedin more detail in reference to FIGS. 9 a-9 b, 10 a-10 b and 11 a-11 b,an embodiment of the supercontinuum fiber comprises a single-mode (i.e.single transverse spatial mode) depressed inner clad fiber.

In general, pump 14 can be any pump capable of producing an opticalpulsed pump signal in a narrow spectral band. There are many differentways to configure the pump pulse for supercontinuum generation dependingon what properties of the supercontinuum source are most relevant ordesirable to a given application. A few general trends are worthclarifying. The peak power of the pump is clearly important, since theorigin of supercontinuum generation depends on the nonlinear interactionof the pump light field with the core glass in the fiber; this dependson the intensity of the pump light in the core, and the overall effectof the nonlinear interaction benefits greatly from higher intensity.Typically, the pump generates very short optical pulses (<1 ps) withhigh peak power at a repetition rate in the tens of MHz. The peak powermust exceed a threshold such that the nonlinear interactions with thesupercontinuum fiber produce supercontinuum. The pulse width may benarrower on the order of femto-seconds or wider. The repetition rate maybe higher or lower.

The center wavelength of the pump relative to the zero dispersionwavelength of the fiber determines the nature and how well the launchedpump pulse generates supercontinuum. The pump may be on the shortwavelength side of ZDW (normal dispersion regime), exactly at the ZDW,or on the long wavelength side of the ZDW (anomalous dispersion regime).Operating at the ZDW enables the pump pulse to propagate along thesupercontinuum fiber without temporal broadening, thus enabling the pumpto interact with extended sections of the fiber while maintaining a highintensity. This can result in highly efficient conversion of pump lightto supercontinuum. Operating the pump in the normal dispersion regimetypically results in temporal broadening, and less supercontinuumgeneration over a narrower spectral band; however, because of the moregradual interaction, the supercontinuum spectra may be smoother and morestable. Operating in the anomalous dispersion regime can also be favoredparticularly when certain types of nonlinear effects are available inthe fiber core. For example, certain nonlinearities coupled withanomalous dispersion may result in soliton formation, which can behighly effective for supercontinuum generation—since solitons propagatealong long lengths of fiber with little or no temporal change. This canresult in efficient supercontinuum generation characterized by solitonpulses. Soliton propagation depends critically on pulse intensity, pulsewidth, and dispersion. Given the richness of the nonlinear effects infibers, many different configurations of the pump pulse (peak intensity,temporal pulse shape, center wavelength) can be designed to takeadvantage of different properties of the supercontinuum fiber.

With this in mind, there is a general approach to optimize the pumpconfiguration given a supercontinuum source that has wide spectralcoverage and high average power in an all-fiber based architecture. Afiber pump source comprising of a short pulse (˜1 ps) and highrepetition rate (>20 MHz) mode-locked laser oscillator and multiplestages of fiber amplifiers, can generate high peak power that is limitedby optical nonlinearities in the doped fiber amplifiers. Beyond acertain limit, the pulse becomes distorted and not effective as a pumpfor supercontinuum generation. So a favorable approach is to select thehighest peak power that can be supported by the given fiber amplifierstages (based on silica or germanate or silicate glass), and thenstretch the temporal pulse width from 1 ps to 10 ps or longer such thatpeak power is maintained over the stretched pulse. This will offer thehighest peak power and largest pump energy available for thesupercontinuum process. To maximize the average output power of thesupercontinum, longer pulses with more energy and high repetition ratesare used such that many high energy pulses are available for thesupercontinuum generation. Practical concerns about the wavelengthcenter are dictated by the dopants and glass used in the fiber-basedpump source, and this has influence on choice of pump laser for a givensupercontinuum fiber in terms of matching the ZDW of the fiber with thepump wavelength, particularly when combined with possibility of solitonpropagation of the pump in the supercontinuum fiber.

Thulium doped, Holmium doped, Thulium-Holmium co-doped silica, silicate,tellurite, and germanate fibers can be used in the pump laser, and areused to fabricate mode locked or q-switched laser oscillators andamplifier stages operating in the 2-micron region. Such pumps deliverpulse widths from ps range to ns or more with high repetition rates (>20MHz), and high average power (10's of Watts). These sources are highlypractical, cost effective, and power scalable for pumping, for example,tellurite fiber based supercontinuum sources—with Watts level or more ofsupercontinuum average power, covering a wide spectral band fromI-micron to 5-micron in an all-fiber architecture.

In general, coupler 16 can be any mechanism for coupling the pump signalinto the supercontinuum fiber including butt-coupling, free space opticsor a fusion-spliced tapered depressed inner clad fiber. As will bedescribed in more detail in reference to FIGS. 12 a-12 b, 13 and 14, atapered depressed inner clad fiber can couple a single-mode pump signalto the supercontinuum fiber with very low loss, approximately 10% asopposed to 50% for free space optics.

The source 10 generates supercontinuum light 20 that spans a definedspectral band having an upper edge of at least 3.5 microns. The band maycover the MIR of 2-5 um, a portion of the MIR, a broader band includingMIR or a portion of the LWIR above 5 microns. The “spectral band” isdefined by a wavelength region in which the output power is generallyspectrally flat (other than at the pump wavelength and near the upperand lower edges). Flatness may be defined as less than 10 dB variationover a sub-band of approximately 1500 nm. The lower and upper edges ofthe spectral band are defined as the shortest and longest wavelengths atwhich the output power is 30 dB down from the output power in thespectrally flat region.

The “spectral band” is also defined by a certain minimum output powerover the band and at the lower and upper edges. The minimum output powerwill depend on the spectral band and the application. For example, for asource configured to generate single-mode supercontinuum over the MIRband from approximately 2 to 5 microns, the total average power from 2-5microns should be at least 150 mW and preferably greater than IW. Thepump-to-supercontinuum efficiency should be at least 5%. The outputpower requirements may be specified over different sub-bands of thespectral band. For example, for 2-5 microns the average integrated powerfrom the visible to 1940 nm>50 mW, 2 to 3.5 microns>50 mW, 3.5 to 5microns>50 mW and >4 microns at least 10 mW minimum.

To achieve the spectral flatness and minimum output power requirementswell into and above the MIR band, the core glass of the supercontinuumfiber must exhibit very low-loss across the spectral band.

Consider a core glass that uses Tellurium oxide as a network former. Intheory a supercontinuum fiber comprising an ideal Tellurium oxide coreglass should support generation of supercontinuum over the MIR band from2 to 5 microns before the absorption features of Tellurium turn off thenonlinear processes that generate supercontinuum.

FIG. 2 plots the transmission spectra of various core glass samples torepresent the evolution in our work to produce supercontinuum fiber withwide spectral coverage in the 1-micron to 5-micron range. A “control”glass TW2-2 is a conventional wet Tellurium-Tungsten glass (no OH—reduction). A first generation glass TZL10-1 is a wetTellurium-Lanthanum glass (no OH— reduction). A second generation glassTZL11-1 is a dry Tellurium-Lanthanum glass (OH— reduced to near zero).

A transmission spectra 30 of the control glass TW2-2 shows hightransmission up to approximately 2.7-micron, at which point thetransmission drops primarily in the 3.3-micron band, but also in the3.7-micron region. These transmission drops are unfavorable towards thegoal of making a highly transparent core glass for supercontinuumgeneration in the mid IR. The absorption in the 3.3-micron band is dueto hydroxide that is embedded in the glass. The absorption at3.7-microns is due to the Tungsten that is added in the glasscomposition to make for a more stable glass. Tungsten has a fundamentalabsorption wavelength of 10.8 microns corresponding to a phonon energypeak. Although the fundamental absorption wavelength lies far above the5 micron upper edge, Tungsten's absorption wavelength corresponding to apeak energy of its 3^(rd) phonon lies at about 3.6 microns. The loss atthe 3^(rd) phonon peak is significant enough to produce the drop in thetransmission spectrum. The loss at the 4^(th) phonon peak of 2.7 micronis sufficiently attenuated that it does not affect the transmissionspectrum.

A transmission spectra 32 of the first generation glass TZL10-1 has no“dip” at 3.7 microns. The Lanthanum used to stabilize the glass has anabsorption wavelength corresponding to a peak energy of its 3^(rd)phonon at about 7.4 micron, well above the edge of the MIR band.However, the transmission drop at 3.3-micron persists since the firstgeneration glass still has Hydroxide incorporation.

A transmission spectra 34 of the second generation glass TZL11-1 showshigh and flat transmission beyond 4-microns, decreasing only due to themulti-phonon edge of the Tellurium oxide. The various steps in glassengineering lead to a core glass with high transmission over the widestpossible range and with no extrinsic absorption features apart from thefundamental multi-phonon edge of the glass. Proper selection of theglass constituents removes the absorption features from the spectralband such that the absorption loss of the multi-phonon edge is very lowwithin the band. Aggressive reduction of OH— produces a final core glassthat is substantially free of OH— (less than 0.1 mole %). OH— reductionto near zero is critical to extend high and flat transmission well intothe MIR band. In certain embodiments the hydroxyl content will be lessthan 0.01 mole % or even 0.001 mole %.

The glass engineering which leads to high transparency and wide spectralcoverage in the mid IR is also highly favorable for the realization of aMid IR supercontinuum source. FIG. 3 a shows a supercontinuum spectra 40using the first generation TZL10-1 core glass. The supercontinuumspectra is relatively narrow in spectral coverage around the 1915 nmwavelength of the pump signal 41. The supercontinuum generation processextends to approximately 3-microns where it abruptly falls due primarilyto the excessive absorption encountered from Hydroxide. Thesupercontinuum process is based on a nonlinear interaction highlydependent on the intensity of the pump light. Any absorption of pumplight or supercontinuum light has the compounded effect of reducingintensity and turning off the nonlinear process as it progresses in thefiber and generates longer wavelength emission. Any absorption in thecore glass will strongly limit the extent of the supercontinuumgeneration. The use of glass constituents to stabilize and strength thefiber that eliminate absorption features is necessary but notsufficient. The absorption mechanisms for both the glass constituentsand OH— must be minimized.

FIG. 3 b shows a supercontinuum spectra 42 using the second generationTZL11-1 core glass in which both the design and processing of the glassremoves all unwanted absorptions. It is clear that the upper edge of thesupercontinuum is shifted to longer wavelengths and cuts off at about 5microns—no longer limited by Hydroxide absorption, and approaching thefundamental multi-phonon edge. With increasing power of the pump signal43 in the core, a supercontinuum spectra 44 where the spectral powerdensity is increased further and the spectral bandwidth is extended onlylimited by the multi-phonon edge on the long wavelength side, and the UVband-edge on the short wavelength side. A comparison of thesupercontinuum spectra for the first and second generation glasses showsthat OH— reduction to near zero is critical to sustain thesupercontinuum generation well into the MIR band.

As discussed, to achieve low loss well into the MIR or possibly LWIRspectral band all of the unwanted absorption mechanisms, particularlythose in the defined output spectral band, must be either removed orsubstantially reduced without compromising glass stability, strength andchemical durability. The proper formulation of the host glass concernsboth what glass constituents are included and what glass constituentsare excluded or minimized.

Our work to improve the optical performance of heavy metal oxide glassesin the MIR and possibly LWIR bands without sacrificing stability,strength and chemical durability has revealed two fundamentalprinciples. First, the oxide glass formulation should not include anyglass constituents (present in more than trace amounts, e.g. >0.2 mole%) having an absorption wavelength corresponding to an energy of thethird phonon peak that is not approximately at or beyond the upper edgeof the spectral band. Otherwise the multi-phonon edge of the host glassmay limit the transmission window. To achieve optical performance asclose as possible to the theoretical limit of the network former, glassconstituents for the intermediate and modifier should be selected whoseabsorption wavelengths at the third phonon peak are longer than that ofthe network former. Second, the heavy metal oxide glass must besubstantially free of OH—. Optimum reduction of OH— is not achieved byusing very high concentrations of halides (e.g. ZnF₂) during the meltthat leave a large residual amount of halide (e.g. F) in the final glasscomposition. Such large concentrations can in fact promote the retentionof moderate amounts of OH by breaking the tellurium oxide bonds creatingmore non-bridging oxygen and producing other unwanted absorbers inaddition to the fact that high concentrations of Fluoride tend to weakenthe glass and reduce its chemical durability.

Our glass formulation only includes glass constituents that provide thenetwork former, intermediate or modifiers, and any halides (for OH—reduction) and any other glass constituent (present in more than traceamounts) whose absorption wavelength for the third phonon peak areapproximately at or beyond the upper edge of the output spectral band.The glass formulation is substantially free of hydroxyl and preferablyincludes at most only a small residual amount of halide. The pre-meltglass formulation suitably includes only a sufficient amount of halideto react with and carry away the hydroxyl during the melt. A non-zeroresidual amount of halide in the glass indicates that substantially allof the hydroxyl is removed. A small residual amount does not degrade thechemical durability of the glass nor does it lead to breakage of oxygenbonds to the network former that would increase absorption in the MIRband and weaken the glass. In many cases it may also be preferred thatthe core glass is substantially free of sodium oxide, which can tend tobond to Hydroxide and make its removal more difficult.

The above glass formulation is specifically for the core glass of thesupercontinuum fiber. The same basic glass formulation holds for thecladding glasses. However, the cladding glasses may be reformulated byvarying the amounts of glass constituents or may include a second glassmodifier to reduce the index of refraction. As above, the glassconstituent selected for the second modifier should have an absorptionwavelength of the third phonon peak approximately at or above the upperedge of the output band. In an embodiment, the second modifier M2O maybe of 0.2 to 47 percent where M is selected from Li, Na, K, Rb and Cs.

FIG. 4 a is a table 50 of the peak phonon energy, the correspondinginherent absorption wavelength and the absorption wavelengthscorresponding to higher order phonon energies for a number of glassconstituents including the common glass formers as well as certainsecond or third component constituents commonly used in producing stableglass formulations.

A phonon is a quantum mechanical description of an elementaryvibrational motion in which a lattice of atoms or molecules uniformlyoscillates at a single frequency. A phonon has an energy or quantaassociated with it which can be excited by the absorption of light withcorresponding energy determined by its wavelength. In solids thatpossess less than perfect periodic structural order, this quanta isbroadened into energies above and below the theoretical peak resultingin an absorption “band” with its peak at that predicted for thetheoretically perfectly ordered solid.

As shown in FIG. 4 b, a multiphonon edge 52 of such a material is alinear combination of absorption bands 54 associated with multiples ofthe energy at the fundamental. With each successive phonon order, theabsorption strength decreases. In addition, successively higher ordersof the fundamental result in bands at progressively shorter wavelengths,which often overlap in their range of wavelengths. The resultingmultiphonon edge often appears as a gradual decrease in transmissiveability for a material as wavelength increases.

For a given spectral band of supercontinuum output, our challenge was tofind glass formers and other glass constituents to produce a stable,strong and chemically durable glass formulation using only materialswhose absorption feature are positioned outside the band. Moreparticularly, the multiphonon edge 52 for each material should be lessthan a threshold absorption level over the spectral band. Based onexperimentation, we have found that the multiphonon edge 52 issufficiently low if the absorption wavelength corresponding to the thirdphonon peak is approximately at or above the upper edge of the desiredspectral band for each glass constituent. The fourth phonon peak issufficiently attenuated that its presence in the spectral band does notintroduce significant losses. In most glass formulations, the absorptionwavelength for the third phonon peak will lie strictly above the upperedge. However, for certain glasses such as W, Ge and Nb the higher orderabsorption bands are weaker and their absorption increases moregradually with wavelength and thus their third phonon peaks may lieslightly below the upper edge, no more than 0.5 um below the edge.

Our next challenge was to provide a final glass formulationsubstantially free of hydroxyl (OH) without degrading the strength,stability and chemical durability of the glass and without creating newabsorbers in the IR band. As with earlier techniques, we introduce ahalide, typically fluoride, into the glass composition that reacts withthe hydroxyl during the melt to form volatile HF that is carried away inthe furnace gas purge. Other halides such as Chloride, Bromide orIodides may be used. The fluoride and chloride are typically introducedas a metal halide such as ZnF₂ or PbF₂.

However, unlike conventional approaches that use large amounts of ZnF₂in the initial glass leaving significant amounts of F₂ in the finalglass, our preferred approach is to limit the initial fluoride contentso that only a small non-zero residual amount of F₂ is present in thefinished glass, typically less than 1 mole % and preferably less than0.5 mol %. To ensure effective OH reduction, it is useful that thefinished glass does contain a non-zero residual amount of F₂. Ourresearch has shown that a large amount of ZnF₂ in the initial glass doesnot improve OH reduction. In fact, substantial residual fluorine contentin the finished glass leads to a breakage of the oxygen bonds with thenetwork former and increased absorption. This breaking of bonds alsoweakens the glass structure leading to increased potential for corrosionand reduced physical strength. By limiting the initial fluoride contentso that only a small residual amount of F₂ is present in the finishedglass, the hydroxyl is removed without breaking the tellurium oxygenbonds or otherwise weakening the glass structure. Even absent efforts tominimize the residual F₂, the content is still at most 15 mole %, andtypically at most 5 mole %, which is less than conventional approaches.

In an embodiment of a supercontinuum source for generating light over anIR spectral band having an upper edge of at least 3.5 microns the coreglass is formed of a heavy metal oxide glass comprising a network formerof 45 to 90 mole percent of an oxide formed from Tellurium (Te), Lead(Pb), Tungsten (W), Tantalum (Ta), Bismuth (Bi), Gallium (Ga), Antimony(Sb), Arsenic (As), Germanium (Ge) or Niobium (Nb) or combinationsthereof, a glass intermediate or modifier of 0.2 to 45 mole percent ofan oxide formed from Lanthanum (La), Tungsten (W), Thallium (TI),Yttrium (Y), Tantalum (Ta), Bismuth (Bi), Gallium (Ga), Antimony (Sb),Arsenic (As), Niobium (Nb). Germanium (Ge), Titanium (Ti), Zirconium(Zr), Magnesium (Mg), Calcium (Ca), Strontium (Sr), Barium (Ba), Zinc(Zn), Lead (Pb) or Cadmium (Cd) or combinations thereof, and a halide of0 to 5 mole percent. The network former, intermediate or modifier, anysaid halide or any other glass constituent of at least 0.2 molepercenteach have an absorption wavelength corresponding to an energy of thethird phonon peak that is approximately at or longer than the edge ofthe IR spectral band. The heavy metal oxide glass is substantially freeof Hydroxide (OH—).

To achieve a spectral band that is only limited by the multiphonon edgeof the network former, the glass formulation includes only anintermediate, modifier, any halide and any other glass constituent whoseabsorption wavelength corresponding to an energy of the third phononpeak is longer than that of the network former.

In an embodiment in which the upper edge of the source's spectral bandis at least approximately 7 microns, the network former is a combinationof lead (Pb) and bismuth (Bi) oxide.

In an embodiment in which the upper edge of the source's spectral bandis at least approximately 6.5 microns, the network former is one ofPb/Bi, Pb/Ga or Pb/Ga/Bi.

In an embodiment in which the upper edge of the source's spectral bandis at least approximately 5.5 microns, the network former is one ofPb/Bi, Pb/Ga, Pb/Ga/Bi or Ta/Ga.

In an embodiment in which the upper edge of the source's spectral bandis at least approximately 5 microns, the network former is one of Pb/Bi,Pb/Ga, Pb/Ga/Bi, Ta/Ga, K/La/Ga or Te.

An embodiment of a process for making a bulk finished glass and using arod-in-tube technique to draw fiber from the finished glass is describedin FIG. 4. A base glass composition is defined (step 60). In thisexample, the base glass composition includes TeO₂ (70%), La₂O₃ (5%) andZnO (25%). Hydroxyl (OH—) is present as an impurity in the constituentpowders, typically at a level of a fraction of a percent. Next a certainpercentage, here 5%, of the ZnO is substituted with a halide, here ZnF₂,(step 62) that acts as the drying agent to remove the OH— during themelt. In general, the percentage of ZnF₂ is preferably selected suchthat the finished glass includes a small non-zero residual amount of theFluoride, enough to ensure that the drying process was not starved ofFluoride and not so much as to break Tellurium Oxide bonds or tootherwise weaken the glass. In different embodiments, the halide mightbe as low as 0.2% and as high as 7% in the initial glass.

Once the glass formulation is set, the oxides and halides are provided,typically in the form of powders, mixed (step 70) and melted (step 72).The time, temperature, purified gas atmosphere and stirring for theglass melt are controlled (step 74). Continuous stirring of the melt hasconsistently produced glasses with very low hydroxyl content, less than0.1 mole % and possibly less than 0.001 mole %. In an embodiment, themixed powders are melted in a gold crucible in a furnace atapproximately 750-950 degrees C. The atmosphere surrounding the cruciblemay be controlled to consist of dry inert gas, oxygen or mixtures ofinert gas and oxygen. The materials within the crucible are maintainedin a liquid state for sufficient time to obtain a homogenous melt. Meltscan be mechanically stirred or bubbled with flowing gas to aid inhomogenization and/or drying.

During the melting and mixing process the fluoride present in the meltwill chemically react with residual hydrogen present in the melt (step76). The fluoride chemical byproducts HF are purged in the exhaust gas(step 78) leaving the glass with no or a minimum amount of hydrogen.Some or all of the initially present zinc fluoride is converted to zincoxide and the resultant glass has a lower concentration of zinc fluoridethan was present in the starting materials. It is desirable to minimizethe zinc fluoride concentration in the glass, since the zinc fluoridereduces the glass transition temperature and makes the glass lessmechanically robust. In this example, the finished glass compositionincludes TeO₂ (70%), La₂O₃ (5%), ZnO (24.5%) and ZnF₂ (0.5%) (step 80).

Glasses obtained may be cast into preheated molds and slowly cooled(annealed) to room temperature in order to relieve stresses (step 82).The mechanical robustness of the resultant glass allows casting ofingots of arbitrary size and shape. An ingot size of approximately1″×1″×5″ is sufficiently large to be used in the fabrication of bulkoptical components or preforms suitable for drawing optical fiber.Alternative methods may be used to form a glass, such as the sol-gelmethod.

An optical fiber can be fabricated from the tellurite glass. Opticalfiber fabricated from the tellurite glass can preserve the glassintrinsic material transmission if the fiber is properly drawn. Onemethod to form optical fiber is the rod-in-tube method. The preformconsists of an inner rod surrounded by an outer tube. These shapes maybe readily fabricated (step 84) from the glass ingot by conventionalglass fabrication techniques, such as mechanical cutting, grinding, andpolishing. An important property of the glass is its resistance tochipping and fracturing, which enables fabrication of the preforms. Thepreform is made by placing a rod with polished outer surfaces inside atube with polished inner and outer surfaces. The inner rod forms thefiber core and the outer tube forms the fiber cladding. The refractiveindex of the core and clad glasses can be manipulated by changing theratio of glass constituents such that any value of numerical aperturefrom 0 to greater than 0.4 can be obtained. One method to change therefractive index is to vary the TeOz to ZnO ratio while leaving theLa₂O₃ level approximately constant. Optical, thermal and mechanicalproperties of the base glass can similarly be adjusted by manipulationof constituent ratios or by the addition of other constituents that haveno unwanted absorptions, such as those listed previously.

To draw the fiber (step 86), the preform can then be placed into afurnace with a controlled atmosphere. The controlled atmosphere may bean inert gas such as nitrogen, argon or helium, or an atmosphere ofoxygen or a combination of gases. The preform may then be heated to atemperature sufficient to soften the glass, causing the core rod andsurrounding tube to fuse together with or without the aid of vacuum. Thepreform pulling temperature is above the glass transition temperature ofapproximately 300 C. The softened and fused glass is subsequently pulledand drawn into fiber. Care must be taken during the drawing to avoidrecrystallization, which can result in the formation of scattering sitesat grain boundaries. A protective coating may be applied to the outercladding surface and the fiber spooled for convenient storage andtransport. The protective coating may be a polymer, metal, carbon, orother coating material. The protective coating helps to preserve theintrinsic strength of the tellurite glass fiber. Fibers drawn from thetelluride glass have demonstrated a tensile strength exceeding 50 KPSI.This high tensile strength facilitates forming a mechanically robustfiber that can be readily handled, spooled, and routed through bulkheadswithout breakage.

Many types of fiber structures may be made in addition to the basicsingle core/single clad geometry. For example, a double clad fiber suchas a depressed inner clad fiber may be made by using two tubessurrounding the core. A fiber with multiple cores may be made. The fibermay include a photonic crystal structure consisting on an array of holeswithin the fiber. The fiber core may be designed to support eithersingle mode or multimode operation. For single mode operation the coredimensions are typically small, no more than several times thewavelength of the light being transmitted. For a multimode fiber, thecore dimensions are typically many times larger than the wavelength ofthe transmitted light. A fiber core diameter of 100 microns may be usedalthough larger and smaller cores may be used depending on theapplication.

Alternative methods of fabricating a fiber may be used in addition tothe rod-in-tube method described above. Preforms may be fabricated byvapor deposition of material on the inner surface of a polished tube.Alternatively, glass in molten form may fill the cavity of a tube. Themolten glass may then be cooled and the resultant assembly used as apreform. Instead of forming the tube by mechanical methods, a tube maybe formed by cooling and solidifying the outer surfaces of a glass ingotand allowing the inner molten regions to drain away.

We will now describe the glass formulation and design process for aparticular embodiment of a heavy metal oxide glass that uses Tellurium(IV) oxide as the network former to provide supercontinuum over aspectral band from 2 to 5 microns. As shown in Table 50 in FIG. 4 a,Tellurium (IV) oxide has a peak phonon energy of 650 cm⁻¹ and acorresponding inherent absorption wavelength of 15.4 microns. Tellurium(IV) oxide has an absorption wavelength at the third phonon peak of 5.1microns. The glass constituents Germanium (Ge), Tungsten (W) and Niobium(Nb) that are commonly used in tellurite glass for MIR applications eachhave an inherent absorption wavelength lower than that of Tellurium (IV)oxide, and absorbing wavelengths at their third phonon peaks less than 4microns, hence they are not viable candidates for our oxide glassformulation. Sodium (Na) and Lead (Pb) do have absorption wavelengthsabove that of Tellurium (IV) oxide but are excluded for other reasons;Sodium inhibits the reduction of OH, severely lowers Tg and weakens theglass and Lead is toxic. In some cases lead may be used.

Lanthanum oxide (La₂O₃) in glass can impart higher glass transitiontemperatures, strength, and durability. Lanthanum oxide is a glassintermediate only forming glass when combined with other constituentssuch as one of the common glass formers Silica dioxide (SiO₂),Phosphorus pentoxide (P₂O₅), Germanium dioxide (GeO₂) or Boron oxide(B₂O₃). Glasses containing lanthanum oxide however are known to be onlymoderately stable over a limited range of composition. Lanthanum oxidein glass is therefore generally limited to a role as a minor constituentcomprising less than a few mole percentage of a given composition.Lanthanum oxide possesses very low phonon energy and even after fourphonons only absorbs at wavelengths over 5 microns. Lanthanum oxidetherefore possesses very desirable characteristics of high Tg, highcorrosion resistance and low UV, Vis and MIR absorption.

To form fiber by the common rod-in-tube technique, a glass preformconsisting of a core rod with a polished outer surface is placed insidea tube with polished inner and outer surface and heated to a temperatureat which the glass rod and tube soften and fuse to be subsequently drawnor pulled to a fiber. A common benchmark for glass stability, ΔT, isdefined as the difference of the peak crystallization temperature Tx andglass transition temperature Tg or ΔT=Tx−Tg as determined by the commoncalorimetric technique Differential Scanning Calorimetry (DSC). Ingeneral a larger ΔT is desirable with a value greater than 100 C oftencited as reasonable for fiber drawing. Glasses containing only telluriumand lanthanum oxides have been made but exhibit very low values of ΔT inthe range of 40 C (Mallawany J. Mater. Sci. (2010) 45: 871-887).

Typically tungsten, niobium or germanium is used to form more stablecompositions with a larger value of ΔT. Again by careful analysis ofTable 50 one realizes tungsten, niobium or germanium containing glassesall have phonon energies larger than TeO₂ and will produce unwantedabsorptions within only as few as three multiples of the peak phononenergy. These materials must then be eliminated from any composition forwhich exceptionally low loss at wavelengths shorter than that oftellurium itself is desired.

Consequently other glass constituents must be found which can stabilizethe Te—La glass compositions. Oxides formed from Magnesium (Mg), Calcium(Ca), Strontium (Sr), Barium (Ba), Zinc (Zn), Lead (Pb) and Cadmium (Cd)may be used to stabilize the Te—La glass composition. Each of theseoxides has an inherent absorption wavelength above that of tellurium.These oxides in combination with tellurium and lanthanum oxides form aglass over an extended compositional region. Addition of these oxides totellurium lanthanum glass compositions leads to increased ΔT values thatare greater than 100 C. A preferred embodiment may use ZnO as it hasbeen demonstrated to form highly stable TeLaZnO glass.

The glass formulation may include various other glass constituents forother glass forming purposes such as to overcome the tendency towardscrystallization and to adjust other physical, thermal and opticalproperties such as Tg, thermal expansion coefficient, or refractiveindex. Any such constituent that is present in the finished glass inother than a de minimus amount (e.g. <0.2 mole %) must not have anabsorption feature with an absorption wavelength of the third phononenergy approximately at or above the IR edge of 5 microns. For example,the base glass can be modified by the addition of other alkali, alkalineearth, transition metal, or heavy metal oxides or halides including Li,K, Rb, Cs, Mg, Ba, Ca, Sr, Y, Ti, Zr, Hf, Nb, Ta, Mo, Ga, In, TI, Pb,As, Ge, Sb and Bi.

Our next challenge was to provide a final glass formulationsubstantially free of hydroxyl (OH) without degrading the strength,stability and chemical durability of the glass and without creating newabsorbers in the IR band. This was achieved by introducing a smallamount of Fluoride into the initial glass composition. The amount ofFluoride is chosen so that at most a residual amount of F₂ is present inthe final glass, typically less than 1 mole % and preferably less than0.5 mol %.

Referring now to FIG. 6, an embodiment of a heavy metal oxide glassformulation 90 for a finished core glass comprises:

a glass network former of Tellurium (IV) oxide TeO₂ 92 of 65 to 9) molepercent;

a glass intermediate of Lanthanum (III) oxide La₂O₃ 94 of 0.2 to 15 molepercent;

a glass modifier MO 96 of 0.2 to 35 mole percent where M is selectedfrom Mg, Ca, Sr, Ba, Zn, Pb and Cd or combinations thereof;

and a halide 98 of 0 to 5 percent,

wherein the oxide glass composition is substantially free of HydroxideOH— and any other glass constituent having an absorption feature with anabsorption wavelength of a third phonon peak that is not approximatelyat or above the upper edge of the supercontinuum. The core glass issuitably substantially free of Sodium Oxide Na₂O.

Once melted into a glass the various constituents become associated withother atoms in a complex way. So TeO₂ becomes a “chain” of Te atoms withfour 0 atoms associated with it “TeO₄” groups or three oxygen “TeO₃”groups or something in between TeO₃₋₁ groups. Zinc fills in spacesbetween Te groups without becoming part of the “chain” and becomes onlyloosely associated with the oxygen or fluorine. Zn changes the shape ofneighboring TeO₄ groups forming TeO₃₋₁ groups with a distortedelectronic cloud. F or O from the Zn move to a position that compensatesfor the distorted electronic cloud to maintain electrical balance.

In an embodiment, the concentration of Lanthanum (III) oxide La₂O₃ 94 is5-15 mole percent. In another embodiment, the concentration is 8-10%. Ingeneral, we have found that it is advantageous for the concentration ofLanthanum (III) oxide to be as high as possible consistent with forminga stable glass. Lanthanum (III) oxide increases the glass transitiontemperature and improves glass mechanical properties.

In an embodiment, the glass modifier MO 96 is ZnO. In an embodiment, theconcentration of ZnO is a combination of ZnO provided in the initialglass pre-melt and ZnO that is formed by converting ZnF₂ or ZnCI duringhydroxyl reduction. In an embodiment, the concentration of ZnO is atleast 10 mole percent. Of the possible modifiers, ZnO has been found toproduce the most stable glass with Lanthanum (III) oxide, which isparticularly important for fiber drawing using the rod-in-tubetechnique.

In an embodiment, the halide 98 is present as a non-zero amount lessthan 1 mole percent, and preferably less than 0.5%. The presence of anon-zero amount of the halide ensures that the hydroxyl reductionprocess during the melt was not starved for a halide to react with thehydroxyl. A small amount of halide ensures that the tellurium oxidebonds are not broken and that the glass is not otherwise weakened by thepresence of a large concentration of halide. In an embodiment, thehalide 98 is Fluoride.

FIG. 7 plots the absorption coefficient versus wavelength for threedifferent glasses: Tellurium Tungsten 100, Tellurium Tungsten w/ OH—reduction 102 and TeLaZnO w/ OH— reduction 104 illustrating first theimprovement in optical performance of effective OH— reduction and thenelimination of any passive constituents whose inherent absorptionwavelength is shorter than that of Tellurium (IV) oxide. The absorptioncoefficient is a measure of the ratio of transmitted power to incidentpower. Tungsten is a standard glass former for Tellurium (IV) Oxide thatis well known to form strong, stable and chemically durable glasses.However, as shown in FIG. 4 a Tungsten has an inherent absorptionwavelength shorter than that of Tellurium (IV) Oxide and the absorptionwavelength of Tungsten corresponding to the third phonon peak lies below5 microns.

As shown, the Tellurium Tungsten glass 100 starts showing someabsorption around 2.7 microns that becomes significant at about 3.0microns. This is due to the absorption features of hydroxyl (OH—). TheTellurium Tungsten glass w/ OH— reduction 102 starts showing someabsorption around 3.0 microns that becomes significant at about 3.7microns. The effective reduction of OH— (without breaking the TeO₂bonds) does significantly extend the bandwidth over which the absorptioncoefficient remains low. However, the presence of Tungsten (W)introduces an absorber at 3.6 microns due to the 3^(rd) phonon energy.These higher order terms result in significant absorption. The TeLaZnOw/ OH— reduction glass 104 starts showing some absorption around 4.0microns that becomes significant at about 4.4 microns, thus extendingthe low loss bandwidth well into the MIR. Because of the “log” scale,these changes in the absorption coefficient are dramatic and havesignificant effects on loss in supercontinuum fibers having lengths inthe meters to tens of meters.

In an embodiment, the oxide glass has an optical loss of less than 2dB/m over the entire spectral range from 0.6 microns to 4.5 microns. Theglass exhibits an optical loss of less than 0.5 dB/m over a spectralsub-band from 0.65 to 4.2 microns. The glass exhibits an optical loss ofless than 0.3 dB/m over a sub-band from 2 microns to 4 microns includingan optical loss of less than 0.3 dB/m due to OH— at approximately 3microns corresponding to the peak absorption of OH—.

FIGS. 8 a and 8 b show the transmission and propagation loss versuswavelength for an exemplary tellurite glass. In this example, thefinished glass formulation comprises TeO₂ (70%), La₂O₃ (5%). ZnO (24.5%)and ZnF₂ (0.5%). The bulk glass and fiber were formed using theprocesses described above.

FIG. 8 a shows the transmission spectrum 110 of a 1.5 mm thick telluriteglass sample prior to fiber draw. The measurement includes the Fresnelreflective losses, so the maximum transmission value is only about 80%.In a broad spectral region from approximately 600 nm to 4000 nm theglass has very low absorption losses. In the short wavelength region theglass maintains some level transmission well into the UV. For example,the sample transmission does not drop to 5% until 353 nm. In the longwavelength region the glass maintains some level of transmission wellinto the mid-infrared. The absorption is negligible until approximately4000 nm. The region from approximately 4000 nm to 5500 nm shows agradual transmission drop. Above 5500 nm the transmission roll off issteeper, but the sample transmission does not drop to 5% until 6380 nm.While in some applications the glass may be useful at shorter or longerwavelengths, most applications for the glass will be in the wavelengthrange of approximately 350 nm to 6400 nm. For applications that requirehigh transmittance or long propagation lengths in the glass, the usefuloperating range is narrower approximately 600 nm to 4500 nm. Thespectral region outside this low loss band may be useful wheretransmittances can be low or propagation lengths short or moderate.

FIG. 8 b illustrates that low loss optical fiber can be drawn from thetellurite glass. The fiber used in this measurement had a core diameterof 70 microns and a cladding outer diameter of 170 microns. Thepropagation loss 112 is less than 0.5 dB/m for IR wavelengths shorterthan approximately 4 microns. Since the thin sample transmissionmeasurements show no absorption features across the near IR region, thefiber drawn from the glass maintains continuous high transmission overthis entire spectral region. Propagation loss begins to rise forwavelengths longer than approximately 4 microns, consistent with thethin sample transmission measurements shown in FIG. 5 a. However, thepropagation loss is still less than 1.5 dB/m for wavelengths longer than4.5 microns. Fiber with propagation losses much higher than 1.5 dB/m isstill useful in applications where the fiber lengths are short or hightransmission is not a requirement.

Referring now to FIGS. 9 a-9 b, 10 a-10 b and 11 a-11 b, in anembodiment the supercontinuum fiber may comprise a depressed inner cladfiber 120 configured to shift the ZDW of the fiber and supportpropagation of the optical pulsed pump signal in only a singletransverse spatial mode to interact nonlinearly with the core glass andgenerate supercontinuum light over the IR spectral band that propagatesin only a single transverse spatial mode. Depressed inner clad fiber 120comprises a core 122 having a zero material dispersion wavelength(ZMDW), a first cladding 124 surrounding the core and a second cladding126 surrounding the first cladding. The core, first cladding and secondcladding having refractive indices n0, n1 and n2, respectively, in whichn1<n2<n0. The core has a radius “a” and the first clad has a radius “b”.

Fiber 120 may include additional cladding layers to enable more refinedwaveguide engineering, such as extending single mode coverage ordispersion shifting or dispersion flattening. In general, additionalcladdings can be favorable for fine-tuning the fiber design. However,there is a practical difficulty in increasing the number of claddings,since it complicates fiber fabrication. Also, there are theoreticalconstraints on the type and physical extent of the claddings to still beeffective. The index of the additional interior claddings generally mustbe lower than the outermost cladding—to ensure that the overallstructure is confining the light properly. Moreover, the physical extentof such additional claddings cannot continue indefinitely and still havea positive effect, since the light field has a limited lateral extentbeyond which additional claddings have no impact.

The depressed inner clad fiber 120 has unique properties that arerelevant to supercontinuum generation including:

(i) The light field is tightly confined in the fiber core, resulting instrong nonlinear effects in the fiber core.

(ii) The dispersion can be significantly manipulated by changing theindex contrast and ratio of claddings and core. Such engineereddispersions could have zero-dispersion wavelength close to the pumpwavelength; can be flattened and have much smaller values as compared tothe single-clad (SC) fibers.

(iii) The fiber can be configured for single mode guidance for the pumpsignal and mid IR wavelengths. Lower modal losses in broad spectralregion can be achieved as compared with single clad fiber.

(iv) The fiber is better than PCF in this application because it is muchsimpler to fabricate, has better power handling because of improvedthermal heat conduction, is less sensitive to bending, is easier tofusion splice with fiber laser pump sources to enable all-fiber system,and has longer term robustness because of monolithic structure with noair holes.

When designing the depressed inner clad fiber 120, one may consider,

Pick suitable glass material for nonlinear core, and index contrasts forcladdings.

SM over some wavelength range (pump, supercontinuum wavelengths).

Shift the zero dispersion to pump wavelength.

Flatten the dispersion slope.

Maximize the intensity in the core for best supercontinuum generation.

In different embodiments for generation of supercontinuum spanning theMIR from approximately 2 to 5 microns, the supercontinuum fibers aredesigned for single mode (SM) cut-off close to a pump wavelength in 1.8to 2.1 micron to optimize pumping propagation in the fiber core, and forSM guidance of the entire MIR supercontinuum in the core. The criterionfor SM guidance is determined by the V-number. In depressed inner cladfiber the condition for SM is:

$\begin{matrix}{{V = {{\frac{2\pi \; a}{\lambda}\sqrt{n_{0}^{2} - n_{2}^{2}}} < 3.503}},} & (1)\end{matrix}$

and for a step-index single clad fiber, SM condition is

$\begin{matrix}{V = {{\frac{2\pi \; a}{\lambda}\sqrt{n_{0}^{2} - n_{1}^{2}}} < {2.405.}}} & (2)\end{matrix}$

In step index fibers, the condition for SM is narrower. In our design,we make use of the depressed inner clad fiber wider mnge of SM guidanceto make the pump and supercontinuum light single mode with low modalloss by design.

In certain embodiments, the fibers have core sizes up to 5 micron,Δn=n₀−n₁ up to 0.16, ratio of inner clad and core S=b/a from 1.5 to 4,ratio R=Δn′/Δn=−0.1 to −0.5 (Δn′=n₁−n₂).

In other embodiments, the fibers have core sizes up to 10 micron,Δn=n₀−n₁ up to 0.4, ratio of inner clad and core S=bia up to 5, ratioR=Δn′/Δn=−0.1 to −0.5 (Δn′=n₁−n₂).

As shown in FIGS. 10 a and 10 b, the dispersion 130 of the depressedinner clad fiber with different Δn and core sizes, S=b/a=2.0, and R=−0.3is flattened and exhibits ZDWs from 1.80 to 2.1 micron. The fiber's ZDQcan be shifted to pump wavelengths in the spectral region larger than1.8 microns with Δn=n₁−n₂ up to 0.16 for tellurite glasses. The zeromaterial dispersion wavelengths (ZMDW) of tellurite glasses are in therange from 2 to 2.5 micron, and it is impossible to shift ZDW shorterthan ZMDW in single-clad single-mode fibers. Dispersions in this designof supercontinuum fiber are also very flat (|ΔD|<20 ps/km/nm overwavelength range 2 to 5 microns) compared with |ΔD|<200 ps/km/nm ofsingle-clad SM fibers.

As shown in FIGS. 11 a and 11 b, the depressed inner clad fiber exhibitsstrong confinement of both the pump 132 at 1.94 micron and thesupercontinuum spectrum in the mid IR from 2 to 5 micron as exhibited bysupercontinuum 134 at 4 micron. Strong confinement is needed to maximizethe nonlinear effect.

Referring now to FIGS. 12, 13 and 14 a and 14 b, in an embodiment thecoupler may comprise a tapered depressed inner clad fiber coupler 140that is fusion spliced between a pump 142 and a supercontinuum fiber144. Pump 142 is configured to produce an optical pulsed pump signal ina given output MFD 146. To maximize pump power, the fiber core and MFDare typically relatively large, e.g. at least 10 micron. The pump signalis also preferably single-mode. Supercontinuum fiber 144 is configuredto receive a single-mode optical pulsed pump signal in a given input MFD148. To ensure single-mode guidance and to provide a high intensity, theMFD is typically relatively small, e.g. less than 5 micron. In thisconfiguration, the input MFD of the supercontinuum fiber 144 is smallerthan the output MFD of the pump 142.

Tapered depressed inner clad fiber coupler 140 comprises a coupler fiber150 having a core 152, a first cladding 154 surrounding the core and asecond cladding 156 surrounding the first cladding. The core, firstcladding and second cladding having refractive indices n0, n1 and n2,respectively, in which n1<n2<n0. The coupler fiber may includeadditional claddings. Coupler fiber 150 is configured with a physicaltaper such that a radius of the core 152 tapers from a radius “a” to asmaller radius a′ such that 2a≈the output MFD 146 of the pump and2a′≈the input MFD 148 of the supercontinuum fiber. The fiber isconfigured with indices of refraction no and n2 that define a numericalaperture (NA) to support propagation of the optical signal in only asingle transverse spatial mode within the spectral band (see equation 1above). The length “l” of the physical taper of the fiber is configuredso that the MFD 158 tapers smoothly (e.g. adiabatically) from theapproximately the output MFD 146 to approximately the input MFD 148. Thefiber is configured with index of refraction n1 and a first claddingradius that tapers from a radius b to b′ so that the taper of the MFD158 approximates the physical taper of the core 152.

Note, the tapered fiber coupler 140 could have higher coupling lossesthan a single clad fiber if the coupler is not properly designed in thetaper section. The refractive index contrast Δn and Δn′, and the ratiobetween inner cladding and core S=b/a must be carefully chosen tominimize loss into the clad. If not properly designed the MFD of thecoupler will not follow the physical taper of the core but will insteadexpand and spread light into the cladding.

Referring now to FIG. 13, an embodiment of a design process forconfiguring the tapered fiber coupler starts with selecting the hostglass for the fiber (step 160). The host glass should be selected tominimize losses at the pump wavelength and to minimize reflection lossesat the fused interfaces between the coupler and the pump and the couplerand the supercontinuum fiber. For a depressed inner clad fiber, thedesigner assumes that a ratio of the radius of the first cladding b tothe radius of the core a is less than some threshold, e.g. 4.5, andassumes that the fiber satisfies the weak guiding condition of (n0−n1)(n1)<<1 (step 162).

Twice the core radius “a” is set to approximately equal the output MFDof the pump and twice the core radius a′ is set to approximately equalthe input MFD of the supercontinuum fiber (step 164). This serves toreduce the losses at the interfaces to the coupler. The designerdetermines the maximum numerical aperture (NA′) that satisfies thesingle-mode criteria at the input core radius a (step 166). For adepressed inner clad fiber the V number is given by equation 1 above.From this one can calculate the maximum NA=√{square root over (n₀ ²−n₂²)}. The designer selects the index of refraction n0 for the core (step168) and selects the smallest index of refraction n2 such that theactual numerical aperture NA<NA′ (step 170) to ensure single-modeguidance throughout the coupler.

The designer sets the length “l” of the physical taper for adiabaticpropagation of the light field of the pump throughout the coupler (step172). In lay terms, the physical taper is sufficiently gradual that thelight field changes slowly enough that light does not leak into thecladding. The designer selected a value for index of refraction n1 andthe ratio S=b/a=b′/a′ so that the taper of the MFD in the couplerfollows the physical taper of the core of the coupler to minimize lossof light into the cladding (step 174). This can be done by simulatingthe MFD along the length of the coupler and determining the percentageof overlap with the core. Proper selection of n1 and S will maximizethis overlap.

The designer calculates the total loss for the coupler design includingreflection losses and MFD mismatch losses at the interfaces to thecoupler and propagation losses into the coupling and compares the totalloss to a threshold (step 176). If the loss is not less than thethreshold, the designer increments the refractive index n2 such that theNA<NA′ (step 178) and repeats steps 172, 174 and 176 until the thresholdcondition is satisfied. Once the condition is satisfied, the designermay or may not elect to refine the core diameters a and a′ and repeatthe design process to try to find a design that satisfied a globalminimum for loss (step 180). Once an acceptable loss is found, thecoupler design is finished (step 182)

As shown in FIGS. 14 a and 14 b, the tapered depressed inner clad fibercoupler exhibits strong confinement of the pump 184 at the interfacebetween the pump and coupler (FIG. 14 a) where the MFD 146 approximatelyequals 2a and at the interface between the coupler and thesupercontinuum fiber (FIG. 14 b) where the MFD 148 approximately equals2a′. Strong confinement is needed to efficiently couple the pump signalfrom the pump to the supercontinuum fiber.

While several illustrative embodiments of the invention have been shownand described, numerous variations and alternate embodiments will occurto those skilled in the art. Such variations and alternate embodimentsare contemplated, and can be made without departing from the spirit andscope of the invention as defined in the appended claims.

We claim:
 1. An IR supercontinuum source for generating light over an IRspectral band having an upper edge of at least 3.5 microns, comprising:a supercontinuum fiber having a core having an optical non-linearitysufficient for supercontinuum generation, said core formed of a heavymetal oxide glass comprising a network former of 45 to 90 mole percentof an oxide formed from Tellurium (Te), Lead (Pb), Tungsten (W),Tantalum (Ta), Bismuth (Bi), Gallium (Ga), Antimony (Sb), Arsenic (As),Germanium (Ge) or Niobium (Nb) or combinations thereof, a glassintermediate or modifier of 0.2 to 45 mole percent of an oxide formedfrom Lanthanum (La), Tungsten (W), Thallium (TI), Yttrium (Y), Tantalum(Ta), Bismuth (Bi), Gallium (Ga), Antimony (Sb), Arsenic (As), Niobium(Nb), Germanium (Ge), Titanium (Ti), Zirconium (Zr), Magnesium (Mg),Calcium (Ca), Strontium (Sr), Barium (Ba), Zinc (Zn), Lead (Pb) orCadmium (Cd) or combinations thereof, and a halide of 0 to 15 molepercent, wherein said network former, intermediate or modifier, and anysaid halide or any other glass constituent of at least 0.2 mole percenteach have an absorption wavelength corresponding to an energy of thethird phonon peak that is approximately at or longer than the upper edgeof the IR spectral band, wherein said heavy metal oxide glass issubstantially free of Hydroxide (OH—); a pump configured to produce anoptical pulsed pump signal; and a coupler that couples the pulsed pumpsignal to the supercontinuum fiber, said supercontinuum fiber configuredto propagate the pulsed pump signal to interact nonlinearly with thesupercontinuum fiber core to generate supercontinuum light that spansthe IR spectral band.
 2. The IR supercontinuum source of claim 1,wherein the absorption wavelengths corresponding to the energy of thethird phonon peak for the intermediate and modifier are longer than theabsorption wavelength corresponding to the energy of the third phononpeak for the network former.
 3. The IR supercontinuum source of claim 1,wherein the halide comprises a non-zero amount of a halide less than 1mole percent.
 4. The IR supercontinuum source of claim 1, whereinsubstantially free is less than 0.1 mole percent.
 5. The IRsupercontinuum source of claim 1, wherein the upper edge is at least 4.5microns, wherein said network former is Tellurium oxide and theintermediate is Lanthanum oxide.
 6. The IR supercontinuum source ofclaim 5, wherein the Lanthanum oxide concentration is at least 5 molepercent; the halide comprises a non-zero amount of Fluoride less than0.5 mole percent, and the modifier MO comprises ZnO.
 7. The IRsupercontinuum source of claim 5, wherein the supercontinuum fiber'score oxide glass exhibits an optical loss of less than 0.3 dB/m over aspectral sub-range from 2 microns to 4 microns.
 8. The IR supercontinuumsource of claim 5, wherein the source produces an integrated averageoutput power of at least 10 mW over 4 to 5 microns.
 9. The IRsupercontinuum source of claim 1, wherein the upper edge is at leastapproximately 7 microns, wherein said network former is a combination oflead (Pb) and bismuth (Bi) oxide.
 10. The IR supercontinuum source ofclaim 1, wherein the upper edge is at least 6.5 microns, wherein saidnetwork former is one of PbIBi, Pb/Ga or Pb/Ga/Bi.
 11. The IRsupercontinuum source of claim 1, wherein the upper edge is at least 5.5microns, wherein said network former is one of Pb/Bi, Pb/Ga, Pb/Ga/Bi orTa/Ga.
 12. The IR supercontinuum source of claim 1, wherein the upperedge is at least 5 microns, wherein said network former is one of Pb/Bi,Pb/Ga, Pb/Ga/Bi, Ta/Ga, KLa/Ga or Te.
 13. The IR supercontinuum sourceof claim 1, wherein the supercontinuum fiber comprises the core oxideglass having a zero material dispersion wavelength (ZMDW), a firstcladding surrounding said core and a second cladding surrounding saidfirst cladding, said core, first cladding and second cladding havingrefractive indices n0, n1 and n2, respectively, in which n1<n2<n0,wherein said supercontinuum fiber is configured to shift a zerodispersion wavelength (ZDW) of the fiber away from the core glass ZMDW;wherein said pump is configured to produce the optical pulsed pumpsignal at the pump wavelength near the fiber's shifted ZDW; wherein saidsupercontinuum fiber is configured to support propagation of the opticalpulsed pump signal in only a single transverse spatial mode to interactnonlinearly with the core glass and generate supercontinuum light overthe IR spectral band that propagates in only a single transverse spatialmode.
 14. The IR supercontinuum source of claim 13, wherein said thepump produces the optical pulsed pump signal with a first mode fielddiameter (MFD) and said supercontinuum fiber receives the optical pulsedpump signal with a smaller second MFD, said coupler comprising: acoupler fiber comprising a core, a first cladding surrounding said coreand a second cladding surrounding said first cladding, said core, firstcladding and second cladding having refractive indices n0, n1 and n2,respectively, in which n1<n2<n0, wherein said fiber is configured with aphysical taper such that a radius of the core tapers from a radius a toa smaller radius a′ such that 2a≈the first MFD and 2a′≈the second MFD;wherein said fiber is configured with indices of refraction n0 and n2that define a numerical aperture to support propagation of the opticalsignal in only a single transverse spatial mode within the spectralband; wherein the length of the physical taper of the fiber isconfigured so that the MFD tapers smoothly from the approximately thefirst MFD to approximately the second MFD; and wherein said fiber isconfigured with index of refraction n1 and a first cladding radius thattapers from a radius b to b′ so that the taper of the MFD approximatesthe physical taper of the core.
 15. The IR supercontinuum source ofclaim 14, wherein said supercontinuum fiber is configured so thatn0−n1>0.1 to provide nonlinearity sufficient for supercontinuumgeneration and said coupler fiber is configured with (n0−n1)/(n1)<<1 andn0−n1<0.05.
 16. The IR supercontinuum source of claim 14, wherein thefirst MFD is at least 10 microns and the second MFD is less than 5microns.
 17. The IR supercontinuum source of claim 1, wherein said thepump produces the optical pulsed pump signal with a first mode fielddiameter (MFD) and said supercontinuum fiber receives the optical pulsedpump signal with a smaller second MFD, wherein said supercontinuum fiberis configured to support propagation of the optical pump signal and thesupercontinuum in only a single transverse spatial mode, said couplercomprising: a coupler fiber comprising a core, a first claddingsurrounding said core and a second cladding surrounding said firstcladding, said core, first cladding and second cladding havingrefractive indices n0, n1 and n2, respectively, in which n1<n2<n0,wherein said fiber is configured with a physical taper such that aradius of the core tapers from a radius a to a smaller radius a′ suchthat 2a≈the first MFD and 2a′≈the second MFD; wherein said fiber isconfigured with indices of refraction n0 and n2 that define a numericalaperture to support propagation of the optical signal in only a singletransverse spatial mode within the spectral band; wherein the length ofthe physical taper of the fiber is configured so that the MFD taperssmoothly from approximately the first MFD to approximately the secondMFD; and wherein said fiber is configured with index of refraction n1and a first cladding radius that tapers from a radius b to b′ so thatthe taper of the MFD approximates the physical taper of the core. 18.The IR supercontinuum source of claim 17, wherein the length of thephysical taper of the fiber is configured so that the optical signalpropagates adiabatically through the coupler.
 19. The IR supercontinuumsource of claim 1, wherein the pump is a fiber pump, the coupler is afiber coupler, and the fiber pump, fiber coupler and supercontinuumfiber are fusion spliced to form an all-fiber IR supercontinuum source.20. The IR supercontinuum source of claim 1, wherein the pump comprisesa fiber pump source and multiple fiber amplifier stages.
 21. An IRsupercontinuum source for generating light over an IR spectral bandhaving an upper edge of at least 3.5 microns, comprising: asupercontinuum fiber having a core glass, a first cladding surroundingsaid core and a second cladding surrounding said first cladding, saidcore, first cladding and second cladding having refractive indices n0,n1 and n2, respectively, in which n1<n2<n0, wherein said fiber isconfigured to receive an optical pulsed pump signal in a first modefield diameter (MFD) and support propagation of the signal in only asingle transverse spatial mode to interact nonlinearly with the coreglass and generate supercontinuum light over the IR spectral band thatpropagates in only a single transverse spatial mode, said core glassformed of a heavy metal oxide glass comprising a network former of 45 to90 mole percent of an oxide formed from Tellurium (Te), Lead (Pb),Tungsten (W), Tantalum (Ta), Bismuth (Bi), Gallium (Ga), Antimony (Sb),Arsenic (As), Germanium (Ge) or Niobium (Nb) or combinations thereof, aglass intermediate or modifier of 0.2 to 45 mole percent of an oxideformed from Lanthanum (La), Tungsten (W), Thallium (TI), Yttrium (Y),Tantalum (Ta), Bismuth (Bi), Gallium (Ga), Antimony (Sb), Arsenic (As),Niobium (Nb), Germanium (Ge), Titanium (Ti) or Zirconium (Zr) Magnesium(Mg), Calcium (Ca), Strontium (Sr), Barium (Ba), Zinc (Zn), Lead (Pb) orCadmium (Cd) or combinations thereof, and a halide of 0 to 15 molepercent, wherein said network former, intermediate or modifier, and anysaid halide or any other glass constituent of at least 0.2 mole percenteach have an absorption wavelength corresponding to an energy of thethird phonon peak that is approximately at or longer than the upper edgeof the IR spectral band, wherein said heavy metal oxide glass issubstantially free of Hydroxide (OH—); a pump configured to produce anoptical pulsed pump signal in a single transverse spatial mode with asecond MFD greater than said first MFD; and a fiber coupler fusionspliced between said pump and said supercontinuum fiber to couple thepulsed pump signal from the second MFD into the smaller first MFD of thesupercontinuum fiber, said fiber coupler comprising a core, a firstcladding surrounding said core and a second cladding surrounding saidfirst cladding, said core, first cladding and second cladding havingrefractive indices n0, n1 and n2, respectively, in which n1<n2<n0,wherein said fiber coupler is configured to support propagation of theoptical pulsed pump signal in only a single transverse spatial modealong a physical taper of the fiber so that a MFD of the coupler tapersfrom approximately the larger second MFD from the pump to approximatelythe smaller first MFD of the supercontinuum fiber.
 22. An IRsupercontinuum source for generating light over an IR spectral bandspanning at least 3 to 5 microns, comprising: a supercontinuum fiberhaving a core having an optical non-linearity sufficient forsupercontinuum generation, said core formed of an oxide glass comprisinga network former of 45 to 90 mole percent of an oxide formed fromTellurium (Te), said Tellurium oxide having an absorption feature withan absorption wavelength corresponding to an energy of the third phononpeak that is longer than 5 microns, a glass intermediate of 0.2 to 45mole percent of an oxide formed from Lanthanum (La), a glass modifier of0.2 to 45 mole percent of an oxide formed from Mg, Ca, Sr. Ba, Zn, Pband Cd or combinations thereof, and a halide of 0 to 5 mole percent,wherein said intermediate and modifier and any said halide each have anabsorption wavelength corresponding to an energy of the third phononpeak that is longer than that of the Tellurium oxide, said oxide glasssubstantially free of Hydroxide (OH—) and any other glass constituenthaving an absorption feature with an absorption wavelength correspondingto a energy of a third phonon peak that is shorter than that of theTellurium oxide; a pump configured to produce an optical pulsed pumpsignal; and a coupler that couples the pulsed pump signal to thesupercontinuum fiber, said supercontinuum fiber configured to propagatethe pulsed pump signal to interact nonlinearly with the supercontinuumfiber core to generate supercontinuum light that spans the IR spectralband of at least 3 to 5 microns.
 23. The IR supercontinuum source ofclaim 22, wherein the Lanthanum oxide concentration is at least 5 molepercent; the halide comprises a non-zero amount of Fluoride less than0.5 mole percent, and the modifier MO comprises ZnO wherein said oxideglass exhibits an optical loss of less than 0.3 dB/m over a spectralsub-range from 2 microns to 4 microns, wherein the source produces anintegrated average output power of at least 10 mW over 4 to 5 microns.24. The IR supercontinuum source of claim 22, wherein the supercontinuumfiber comprises the core Tellurium oxide glass having a zero materialdispersion wavelength (ZMDW), a first cladding surrounding said core anda second cladding surrounding said first cladding, said core, firstcladding and second cladding having refractive indices n0, n1 and n2,respectively, in which n1<n2<n0, wherein said supercontinuum fiber isconfigured to shift a zero dispersion wavelength (ZDW) of the fiber awayfrom the core glass ZMDW; wherein said pump is configured to produce theoptical pulsed pump signal at the pump wavelength near the fiber'sshifted ZDW; wherein said supercontinuum fiber is configured to supportpropagation of the optical pulsed pump signal in only a singletransverse spatial mode to interact nonlinearly with the core glass andgenerate supercontinuum light over the IR spectral band that propagatesin only a single transverse spatial mode.
 25. An IR supercontinuumsource, comprising: a supercontinuum fiber comprising a core, a firstcladding surrounding said core and a second cladding surrounding saidfirst cladding, said core, first cladding and second cladding havingrefractive indices n0, n1 and n2, respectively, in which n1<n2<n0,wherein said core, first cladding and second cladding are formed from aheavy metal oxide glass, said core glass having a zero materialdispersion wavelength (ZMDW) and a non-linearity sufficient forsupercontinuum generation; wherein said supercontinuum fiber isconfigured to shift a zero dispersion wavelength (ZDW) of the fiber awayfrom the core glass ZMDW; a pump configured to produce a pulsed pumpsignal at a pump wavelength near the fiber's shifted ZDW; and a couplerthat couples the pulsed pump signal to the supercontinuum fiber, whereinsaid supercontinuum fiber is configured to support propagation of thepulsed pump signal in only a single transverse spatial mode to interactnonlinearly with the core glass and generate supercontinuum light overan IR spectral band that propagates in only a single transverse spatialmode.
 26. The IR supercontinuum source of claim 25, wherein said thepump produces the optical pulsed pump signal with a first mode fielddiameter (MFD) of at least 10 microns and said supercontinuum fiberreceives the optical pulsed pump signal with a smaller second MFD ofless than 5 microns, wherein said supercontinuum fiber is configuredwith n0−n1>0.1 to provide nonlinearity for supercontinuum generation andis configured to support propagation of the optical pump signal and thesupercontinuum in only a single transverse spatial mode, said couplercomprising: a coupler fiber comprising a core, a first claddingsurrounding said core and a second cladding surrounding said firstcladding, said core, first cladding and second cladding havingrefractive indices n0, n1 and n2, respectively, in which n1<n2<n0,wherein with (n0−n1)/(n1)<<1 and n0−n1<0.05, wherein said fiber isconfigured with a physical taper such that a radius of the core tapersfrom a radius a to a smaller radius a′ such that 2a=the first MFD and2a′≈the second MFD; wherein said fiber is configured with indices ofrefraction n0 and n2 that define a numerical aperture to supportpropagation of the optical signal in only a single transverse spatialmode within the spectral band; wherein the length of the physical taperof the fiber is configured so that the MFD tapers smoothly fromapproximately the first MFD to approximately the second MFD; and whereinsaid fiber is configured with index of refraction n1 and a firstcladding radius that tapers from a radius b to b′ so that the taper ofthe MFD approximates the physical taper of the core.
 27. An IRsupercontinuum source for generating light over an IR spectral bandhaving an upper edge of at least 3.5 microns, comprising: asupercontinuum fiber having a heavy metal oxide core glass, wherein saidfiber is configured to receive an optical pulsed pump signal in a firstmode field diameter (MFD) and support propagation of the signal in onlya single transverse spatial mode to interact nonlinearly with the coreglass and generate supercontinuum light over the IR spectral band thatpropagates in only a single transverse spatial mode, a pump configuredto produce an optical pulsed pump signal in a single transverse spatialmode with a second MFD greater than said first MFD; and a fiber couplerfusion spliced between said pump and said supercontinuum fiber to couplethe pulsed pump signal from the second MFD into the smaller first MFD ofthe supercontinuum fiber, said fiber coupler comprising a core, a firstcladding surrounding said core and a second cladding surrounding saidfirst cladding, said core, first cladding and second cladding havingrefractive indices n0, n1 and n2, respectively, in which n1<n2<n0,wherein said fiber coupler is configured to support propagation of theoptical pulsed pump signal in only a single transverse spatial modealong a physical taper of the fiber so that a MFD of the coupler tapersfrom approximately the larger second MFD from the pump to approximatelythe smaller first MFD of the supercontinuum fiber.